ライフサイエンスコーパス: holey

1 Recent reports on holey graphene showed that holey 2D nanosheets can outperform their intact counterp

2 f two-dimensional (2D) nanosheets results in holey 2D nanosheets that have abundant edge atoms.

3 tion perspectives, it is desirable to obtain holey 2D nanosheets with defined hole morphology and hol

4 y qualitative and quantitative properties of holey adaptive landscapes which may be related to the pa

5 he patch specifically and observe asymmetric holey capsids by cryo-EM reconstruction.

6 bes how to create a grid surface coated with holey carbon by first inducing holes in a Formvar film t

7 However, difficulties in preparing holey carbon cryo-EM grids with low vesicle heterogeneit

8 nding DNA-affinity superlattice for covering holey carbon cryo-EM grids.

9 suring force displacement characteristics of holey carbon EM-grids, we found that their effective spr

10 in particular crystalline silicon wafers and holey carbon films.

11 ituted in nanodiscs was applied to a cryo-EM holey carbon grid to define its composition.

12 It takes 4-5 h to make several hundred holey carbon grids and about 1 h to make the frozen-hydr

13 a Formvar film to act as a template for the holey carbon that is stable under cryo-electron microsco

14 An appropriate image of resulting ("holey") fitness landscapes is a (multidimensional) flat

15 es, consisting of interconnected N,S-codoped holey graphene (HG) sheets.

16 aximum of 1.50 at 300 K, higher than that of holey graphene (ZT = 1.13), gamma-graphyne (ZT = 0.48),

17 Herein, we report hygroscopic holey graphene aerogel fibers (LiCl@HGAFs) with integrat

18 , an electrode material based on anisotropic holey graphene aerogel is synthesized with improved ion

19 th a high reversibility by using B,N-codoped holey graphene as a highly efficient catalyst for CO2 re

20 systematically tailoring the porosity in the holey graphene backbone, charge transport in the composi

21 twork using the nitrogen, sulfur, dual-doped holey graphene framework as a model electrode to underst

22 e found that the nitrogen, sulfur dual-doped holey graphene framework catalyst could help accelerate

23 hways as well as a high packing density, the holey graphene framework electrode can deliver a gravime

24 Here we report a three-dimensional holey graphene framework with a hierarchical porous stru

25 Recent reports on holey graphene showed that holey 2D nanosheets can outpe

26 emerged as a highly versatile alternative to holey graphene.

27 eport the design of a three-dimensional (3D) holey-graphene/niobia (Nb2O5) composite for ultrahigh-ra

28 carbon, carbon nanotubes and crosslinked or holey graphenes are used exclusively as the active elect

29 Such colossal ZT values make holey graphyne an appealing p-type thermoelectric materi

30 Our findings disclose that holey graphyne has a direct bandgap of 1.00 eV using the

31 Besides that, holey graphyne is a potential HER catalyst with a low ov

32 The formation energy of holey graphyne turns out to be - 8.46 eV/atom, comparabl

33 n catalytic activity of recently synthesized holey graphyne.

34 ism, revealing abundant oxygen vacancies and holey lamellar framework contribute to the ultra-high ca

35 Now, a holey lamellar high entropy oxide (HEO) Co(0.2) Ni(0.2)

36 amework) scenario of biological evolution on holey landscapes assuming that it starts on a genotype f

37 rding to the properties of the corresponding holey landscapes.

38 tent with evolution across high-dimensional "holey landscapes." This suggests that the leading concep

39 With holey MgO nanosheets as an example, the protected Li ano

40 Here, parallelly aligned holey nanosheets on a Li metal anode are reported to sim

41 Benefiting from the unique porous holey nanostructure and high catalytic activity of the c

42 Here, we report a Fe/Cu diatomic catalyst on holey nitrogen-doped graphene which exhibits high cataly

43 We find that these holey oxide nanosheets exhibit strong mechanical stabili

44 These holey oxide nanosheets represent a promising material pl

45 Thus, instead of a holey protein array, the experimental model presented he

46 translational symmetry allows the six-petal holey silicon to achieve the topological phase transitio

47 erse phonon polarizations. Here we present a holey silicon-based topological insulator design, in whi

48 This concept is demonstrated for a holey-structured acoustic metamaterial in water at 200-3

49 strategy for versatile synthesis of various holey transition metal oxide nanosheets with adjustable